|| Measuring the coefficients of friction . One straightforward way to measure the coefficients of friction between a box and a wooden surface is illustrated in Figure 5.55 . The sheet of wood can be raised by pivoting it about one edge. It is first raised to an angle 81 (which is measured) for which the box just begins to slide downward. The sheet is then immediately lowered to an angle 92 (which is also measured) for which the box slides with constant speed down the sheet. Apply Newton’s second law to the box in both cases to find the coefficients of kinetic and static friction between it and the wooden sheet in terms of the measured angles θ1 and θ 2 . Figure 5.55 Problem 34.
|| Measuring the coefficients of friction . One straightforward way to measure the coefficients of friction between a box and a wooden surface is illustrated in Figure 5.55 . The sheet of wood can be raised by pivoting it about one edge. It is first raised to an angle 81 (which is measured) for which the box just begins to slide downward. The sheet is then immediately lowered to an angle 92 (which is also measured) for which the box slides with constant speed down the sheet. Apply Newton’s second law to the box in both cases to find the coefficients of kinetic and static friction between it and the wooden sheet in terms of the measured angles θ1 and θ 2 . Figure 5.55 Problem 34.
|| Measuring the coefficients of friction. One straightforward way to measure the coefficients of friction between a box and a wooden surface is illustrated in Figure 5.55. The sheet of wood can be raised by pivoting it about one edge. It is first raised to an angle 81 (which is measured) for which the box just begins to slide downward. The sheet is then immediately lowered to an angle 92 (which is also measured) for which the box slides with constant speed down the sheet. Apply Newton’s second law to the box in both cases to find the coefficients of kinetic and static friction between it and the wooden sheet in terms of the measured angles θ1 and θ2.
Paraxial design of a field flattener. Imagine your optical system has Petzal curvature of the field with radius
p. In Module 1 of Course 1, a homework problem asked you to derive the paraxial focus shift along the axis
when a slab of glass was inserted in a converging cone of rays. Find or re-derive that result, then use it to
calculate the paraxial radius of curvature of a field flattener of refractive index n that will correct the observed
Petzval. Assume that the side of the flattener facing the image plane is plano. What is the required radius of
the plano-convex field flattener? (p written as rho )
3.37(a) Five free electrons exist in a three-dimensional infinite potential well with all three widths equal to \( a = 12 \, \text{Å} \). Determine the Fermi energy level at \( T = 0 \, \text{K} \). (b) Repeat part (a) for 13 electrons.
Book: Semiconductor Physics and Devices 4th ed, NeamanChapter-3Please expert answer only. don't give gpt-generated answers, & please clear the concept of quantum states for determining nx, ny, nz to determine E, as I don't have much idea about that topic.
3.37(a) Five free electrons exist in a three-dimensional infinite potential well with all three widths equal to \( a = 12 \, \text{Å} \). Determine the Fermi energy level at \( T = 0 \, \text{K} \). (b) Repeat part (a) for 13 electrons.
Book: Semiconductor Physics and Devices 4th ed, NeamanChapter-3Please expert answer only. don't give gpt-generated answers, & please clear the concept of quantum states for determining nx, ny, nz to determine E, as I don't have much idea about that topic.
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